It is clear from the above discussion, that if \(y_t\)  would be,
say, a factor of 5 smaller, the NP coupled to the top could be a factor of 5 heavier while the
fine tuning \(\Delta _{\rm FT}\)  would remain the same and the same is true if the top-Yukawa contribution is cut off significantly earlier than other corrections. This is illustrated in Fig. REF , where the NP contributions to the Higgs mass term from the
top- , \(W\) - , \(Z\) - , and Higgs sectors, normalized to \(m_H\) , are presented – the latter reading [1]} (\(B=W,Z,H\) )
\((\Delta m_H^2)_B = \frac{3}{2} g_B^2 \frac{\Lambda _{\rm NP}^2}{16 \pi ^2}\,,\) 
